The nucleon \(p_T\)  distributions are necessary inputs for computing \(p_T\)  distributions of light nuclei in our method.
We here use the blast-wave model to get invariant \(p_T\)  distribution functions of protons by fitting the proton experimental data in Ref. [1]}.
The blast-wave function [2]} is given as
\(\frac{d^{2}N}{2\pi p_{T}dp_{T}dy} \propto && \int _{0}^{R} r dr m_T I_0 \left(\frac{p_Tsinh\rho }{T_{kin}}\right) \nonumber \\&& ~~~~~ \times K_1\left(\frac{m_Tcosh\rho }{T_{kin}}\right) , \) 
